Nanorheology of confined polymer films

ORAL

Abstract

Liquid films with a non-uniform thickness flatten in order minimize surface energy, a process driven by surface tension and mediated by viscosity. For a viscous thin film, the time evolution of the film height profile is accurately described with lubrication theory by the capillary-driven thin film equation. Previous experiments have successfully applied the thin film equation to measure the rheological properties of polymeric liquids. Here we probe confinement effects in thin polymer films. We measure the viscosity by tracking the levelling of surface perturbations with AFM. For films with thicknesses thinner than the end-to-end distance of the molecule we observe deviations from a thin film model with bulk viscosity.

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Authors

  • Paul Fowler

    • Department of Physics & Astronomy and the Brockhouse Institute for Materials Research, McMaster University, Hamilton, ON, Canada
    • Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada, L8S 4M1

  • Mark Ilton

    • Department of Physics & Astronomy and the Brockhouse Institute for Materials Research, McMaster University, Hamilton, ON, Canada
    • Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada, L8S 4M1

  • Joshua D. McGraw

    • Département de Physique, Ecole Normale Supérieure / PSL Research University, CNRS, 24 rue Lhomond, 75005 Paris, France

  • Kari Dalnoki-Veress

    • Department of Physics & Astronomy and the Brockhouse Institute for Materials Research, McMaster University, Hamilton, ON, Canada
    • McMaster University
    • Department of Physics & Astronomy, McMaster University, Hamilton, Ontario, Canada, L8S 4M1
    • Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, Canada, L8S 4M1